WO2019213163A1 - Dispositif de conditionnement de mode optique mmf - Google Patents
Dispositif de conditionnement de mode optique mmf Download PDFInfo
- Publication number
- WO2019213163A1 WO2019213163A1 PCT/US2019/030047 US2019030047W WO2019213163A1 WO 2019213163 A1 WO2019213163 A1 WO 2019213163A1 US 2019030047 W US2019030047 W US 2019030047W WO 2019213163 A1 WO2019213163 A1 WO 2019213163A1
- Authority
- WO
- WIPO (PCT)
- Prior art keywords
- waveguide
- optical device
- optical
- fiber
- index
- Prior art date
Links
Classifications
-
- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B6/00—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
- G02B6/02—Optical fibres with cladding with or without a coating
- G02B6/028—Optical fibres with cladding with or without a coating with core or cladding having graded refractive index
- G02B6/0281—Graded index region forming part of the central core segment, e.g. alpha profile, triangular, trapezoidal core
-
- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B6/00—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
- G02B6/02—Optical fibres with cladding with or without a coating
- G02B6/028—Optical fibres with cladding with or without a coating with core or cladding having graded refractive index
- G02B6/0288—Multimode fibre, e.g. graded index core for compensating modal dispersion
-
- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B6/00—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
- G02B6/10—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings of the optical waveguide type
- G02B6/14—Mode converters
-
- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B6/00—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
- G02B6/24—Coupling light guides
- G02B6/26—Optical coupling means
- G02B6/262—Optical details of coupling light into, or out of, or between fibre ends, e.g. special fibre end shapes or associated optical elements
-
- G—PHYSICS
- G02—OPTICS
- G02B—OPTICAL ELEMENTS, SYSTEMS OR APPARATUS
- G02B6/00—Light guides; Structural details of arrangements comprising light guides and other optical elements, e.g. couplings
- G02B6/24—Coupling light guides
- G02B6/26—Optical coupling means
- G02B6/268—Optical coupling means for modal dispersion control, e.g. concatenation of light guides having different modal dispersion properties
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- H—ELECTRICITY
- H04—ELECTRIC COMMUNICATION TECHNIQUE
- H04B—TRANSMISSION
- H04B10/00—Transmission systems employing electromagnetic waves other than radio-waves, e.g. infrared, visible or ultraviolet light, or employing corpuscular radiation, e.g. quantum communication
- H04B10/25—Arrangements specific to fibre transmission
- H04B10/2581—Multimode transmission
Definitions
- the present disclosure generally relates to transmission of optical signals in multimode optical fibers (MMF).
- MMF multimode optical fibers
- Multi -mode optical fiber is a type of optical fiber mostly used for communication over short distances, such as within a building or on a campus.
- Multi-mode fiber has a relatively large core diameter that enables multiple light modes to be propagated and limits the maximum length of a transmission link because of modal dispersion. Because of its relatively high capacity and reliability, multi-mode optical fiber generally is used for backbone applications in buildings, although there are other applications for multi-mode fibers.
- the present disclosure generally relates to transmission of optical signals in multimode optical fibers (MMF).
- MMF multimode optical fibers
- an optical device may include a waveguide having a core index of refraction that decreases along a length of the waveguide and an edge index of refraction of the waveguide that is substantially constant along the length of the waveguide.
- the optical device may be a radial symmetric waveguide.
- the optical device may be a fiber stub or a graded-index optic.
- the optical device may be positioned mid-span in an optical fiber.
- the optical device may be optically coupled to a first fiber core and a second fiber core.
- the optical device may include a constant diameter between the first fiber core and the second fiber core. The constant diameter may correspond to a diameter of the first fiber core and a diameter of the second fiber core.
- the optical device may be mechanically coupled to a first fiber core and a second fiber core.
- the waveguide may decrease dispersion of the optical signals travelling through the fiber cores.
- the central rays of optical signals travelling through the waveguide may be refracted towards higher radii while the outer rays propagate unaffected.
- an optical fiber may include the optical device including some or all of the aspects described above.
- the optical device may be positioned between a first portion of the optical fiber and a second portion of the optical fiber.
- the optical device may be positioned between a first end of the optical fiber and a second end of the optical fiber.
- the optical device and the optical fiber may be configured to propagate multi-mode optical signals and/or shortwave optical signals.
- an optical device may include a waveguide having a first index of refraction proximate a center of the waveguide that decreases along a length of the waveguide and a second index of refection of the waveguide proximate a periphery of the waveguide that is constant along the length of the waveguide.
- the optical device may be a radial symmetric waveguide, a fiber stub or a graded-index optic.
- the optical device may be positioned mid-span in an optical fiber.
- the optical device may be optically coupled to a first fiber core and a second fiber core and the optical device decreases dispersion of the optical signals travelling through the fiber cores.
- the central rays of optical signals travelling through the optical device may be refracted towards higher radii while the outer rays propagate unaffected.
- Figure l is a schematic view of an example optical device.
- Figure 2 is a schematic view of the refractive index profile of the optical device of Figure 1
- Multi -mode optical fiber is a type of optical fiber mostly used for communication over short distances, such as within a building or on a campus.
- Multi-mode fiber has a relatively large core diameter that enables multiple light modes to be propagated and limits the maximum length of a transmission link because of modal dispersion. Because of its relatively high capacity and reliability, multi-mode optical fiber generally is used for backbone applications in buildings.
- multi-mode optical fibers have much larger core diameters when compared to single-mode optical fibers.
- multi-mode optical fibers typically have core diameters in the range of 50-100 micrometers, and also typically carry relatively larger wavelengths of light it. Because of the larger core and also the capability of using a large numerical aperture, multi-mode fibers generally have a higher "light-gathering" capacity than single-mode fiber. In practical terms, the larger core size simplifies connections and also allows the use of lower-cost electronics such as light-emitting diodes (LEDs) and vertical-cavity surface-emitting lasers (VCSELs). In some configurations, multimode lasers may operate at 850 nm and 1300 nm wavelengths.
- single-mode fibers used in telecommunications typically operate at 1310 or 1550 nm.
- the multi-mode fiber bandwidth-distance product limit is lower. Because multi-mode fiber has a larger core-size than single-mode fiber, it supports more than one propagation mode. Accordingly, multi-mode fiber is limited by modal dispersion, while single mode fiber generally is not.
- the light sources sometimes used with multi-mode fiber produce a range of wavelengths and these each propagate at different speeds.
- chromatic dispersion is the phenomenon in which the phase velocity of a wave depends on its frequency. Media having this common property may be termed a dispersive media.
- This chromatic dispersion is another limit to the useful length for multi-mode fiber optic cable.
- the light sources used to drive single-mode fibers generally produce coherent light of a single wavelength. Because of the combined modal and chromatic dispersion, multi-mode fiber has higher pulse spreading rates than single mode fiber, limiting multi -mode fiber’s information transmission capacity.
- the length of multi-mode fibers are generally more limited than the length of single mode fibers.
- inventions that permit using multimode fibers over longer distances while using standard transceivers. Additionally or alternatively, embodiments may be implemented to maintain the long reaches possible with mode conditioned transceivers in datacenters with impairments in their fiber plant.
- the disclosed embodiments include standalone optical devices that may be implemented with conventional optical transmitters and transceivers.
- the optical device may be distinct from the transmitter. Additionally or alternatively, the optical device may be small enough to be added to a fiber panel that could take an unconditioned modal pattern in a multi-mode fiber and convert it to a mode pattern that can propagate long distances.
- Some embodiments may be implemented to create a mode conditioned launch property in an already installed standard emission transceiver. Such implementations may be useful to maintain the existing optical fiber length when upgrading to a higher line rate. Additionally or alternatively, implementations may be used when a mode conditioned transceiver is not meeting the expected length benefit due to flaws in the existing fiber panel (e.g., poorly aligned connectors on a patch panel causing mode coupling to a faster central ray). Additionally or alternatively, the described embodiments may be implemented to recondition the optical power in optical fibers into the proper modes, restoring the intended target reach.
- a radial symmetric waveguide may be implemented.
- the core index of refraction of the radial symmetric waveguide may decrease along its length while the index of refection at the edge stays constant.
- the central rays may be refracted towards higher radii while the outer rays propagate unaffected.
- the radial symmetric waveguide could be fabricated as a fiber stub or as a graded-index optic.
- the radial symmetric waveguide may be positioned between two standard optical fibers. The radial symmetric waveguide may decrease dispersion of the optical signals travelling through multimode optical fibers, thereby increasing the length that multimode optical fibers may be used without decreasing signal quality.
- the radial symmetric waveguide may be implemented as an optical device that does not require electrical power.
- the radial symmetric waveguide may increase the distances that optical signals may be transmitted through multimode optical fibers without requiring modifications to existing optical fibers, transceivers, or lasers.
- Figure 1 illustrates a schematic view of an example optical device 100.
- the optical device 100 may be positioned mid-span in an optical fiber. In other configurations, the optical device 100 may be positioned between two standard optical fibers. Accordingly, the optical device 100 may be optically and/or mechanically coupled to a first fiber core 102 and a second fiber core 104.
- the fiber cores 102, 104 may be multimode fiber cores.
- the optical device 100 may include a waveguide 106 positioned between and optically coupled to the fiber cores 102, 104.
- the waveguide 106 may be fabricated as a fiber stub or as a graded- index optic. In some configurations, the waveguide 106 may be a radial symmetric waveguide or radially symmetrical waveguide.
- the core index of refraction of the waveguide 106 may decrease along its length.
- the core index of refraction may refer to an index of refraction positioned at or a proximate to a center of the waveguide 106. Additionally or alternatively, the core index of refraction may refer to an index of refraction positioned at or a proximate to a longitudinal axis of the waveguide 106.
- the edge index of refection of the waveguide 106 may stay relatively constant.
- the edge index of refraction may refer to an index of refraction positioned at or a proximate to the edge or periphery of the waveguide 106.
- the central rays of the optical signals travelling through the waveguide 106 may be refracted towards higher radii while the outer rays propagate unaffected.
- the optical device 100 and the waveguide 106 may decrease dispersion of the optical signals travelling through the fiber cores 102, 104, thereby increasing the length that multimode optical fibers may be used without decreasing signal quality.
- the waveguide 106 may be implemented as an optical device that does not require electrical power.
- the optical device 100 may increase the distances that optical signals may be transmitted through multimode optical fibers without requiring modifications to existing optical fibers, transceivers, or lasers.
- the diameter of the waveguide 106 may be similar or the same as the diameter of the fiber cores 102, 104. As shown, the waveguide 106 includes a relatively constant diameter between the fiber cores 102, 104, and is generally aligned in a position between the fiber cores 102, 104. Although the diameter of the waveguide 106 is relatively constant, the index of refraction of the waveguide 106 is graded, thus it changes over the length of the waveguide 106. In some configurations, the diameter of the fiber cores 102, 104 and/or the waveguide 106 may be between 50-100 micrometers.
- Figure 2 illustrates a schematic view of the refractive index profile of the optical device 100.
- Figure 2 illustrates the changes of the refractive index profile of the waveguide 106 along the propagation direction of the optical signals.
- the core index of refraction of the waveguide 106 decreases along its length and the index of refraction at the edge or proximate the edge of the waveguide 106 stays relatively constant.
- Figure 2 includes example refractive index profiles 202a, 202b, 202c, 202d.
- Each of the refractive index profiles 202a-d includes a refractive index at a corresponding core 204a, 204b, 204c, 204d of the waveguide 106.
- the index of refraction at the cores 204a-d decreases along the length of the waveguide 106 in the propagation direction.
- the index of refraction is largest at the core 204a of the index profile 202a, the index of refraction is relatively smaller at the core 204b of the index profile 202b, the index of refraction is further smaller at the core 204c of the index profile 202c, and the index of refraction is smallest at the core 204d of the index profile 202d.
- Each of the refractive index profiles 202a-d includes a refractive index at corresponding edges 206a, 206b, 206c, 206d of the waveguide 106.
- the index of refraction stays relatively constant at the edges 206a-d along the length of the waveguide 106 in the propagation direction.
- the central rays may be refracted towards higher radii while the outer rays propagate unaffected. This changes the distribution of light within the waveguide by guiding the light into the ring-shaped region of higher refractive index. This produces a ring-shaped modal pattern which is more conducive to propagating long distances.
- the optical device 100 may be positioned mid-span in an optical fiber.
- the optical fiber may be a multimode optical fiber.
- the optical fiber may be may be 1 km, 300 meters, 100 meters, 70 meters in length or less.
- the optical device 100 may be implemented proximate or inside an optoelectronic transceiver.
- an optical fiber may include the optical device 100.
- the optical device 100 may be positioned between a first portion of the optical fiber and a second portion of the optical fiber.
- the optical device 100 may be positioned between a first end of the optical fiber and a second end of the optical fiber.
- the optical fiber may be a multi -mode optical fiber.
- the optical device 100 may be a multi- mode optical device configured to receive, transmit, or propagate multi-mode optical signals. Additionally or alternatively, the optical fiber may be a shortwave optical fiber configured to receive, transmit, or propagate shortwave optical signals (e.g., optical signals in a shortwave spectrum range).
- the optical device 100 may be a shortwave optical device configured to receive, transmit, or propagate shortwave optical signals (e.g., optical signals in a shortwave spectrum range).
- an optical device may include a waveguide having a core index of refraction that decreases along a length of the waveguide and an edge index of refraction of the waveguide that is substantially constant along the length of the waveguide.
- the optical device may be a radial symmetric waveguide.
- the optical device may be a fiber stub or a graded-index optic.
- the optical device may be positioned mid-span in an optical fiber.
- the optical device may be optically coupled to a first fiber core and a second fiber core.
- the optical device may include a constant diameter between the first fiber core and the second fiber core. The constant diameter may correspond to a diameter of the first fiber core and a diameter of the second fiber core.
- the optical device may be mechanically coupled to a first fiber core and a second fiber core.
- an optical fiber may include the optical device including some or all of the aspects described above.
- the optical device may be positioned between a first portion of the optical fiber and a second portion of the optical fiber.
- the optical device may be positioned between a first end of the optical fiber and a second end of the optical fiber.
- the optical device and the optical fiber may be configured to propagate multi-mode optical signals and/or shortwave optical signals.
- an optical device may include a waveguide having a first index of refraction proximate a center of the waveguide that decreases along a length of the waveguide and a second index of refection of the waveguide proximate a periphery of the waveguide that is constant along the length of the waveguide.
- the optical device may be a radial symmetric waveguide, a fiber stub or a graded-index optic.
- the optical device may be positioned mid-span in an optical fiber.
- the optical device may be optically coupled to a first fiber core and a second fiber core and the optical device decreases dispersion of the optical signals travelling through the fiber cores.
- the central rays of optical signals travelling through the optical device may be refracted towards higher radii while the outer rays propagate unaffected.
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- Physics & Mathematics (AREA)
- General Physics & Mathematics (AREA)
- Optics & Photonics (AREA)
- Chemical & Material Sciences (AREA)
- Dispersion Chemistry (AREA)
- Electromagnetism (AREA)
- Engineering & Computer Science (AREA)
- Computer Networks & Wireless Communication (AREA)
- Signal Processing (AREA)
- Optical Couplings Of Light Guides (AREA)
Abstract
Dans un exemple, la présente invention concerne un dispositif optique qui peut comprendre un guide d'ondes ayant un indice de réfraction de cœur qui diminue sur une longueur du guide d'ondes et un indice de réfraction de bord dudit guide d'ondes qui est constant sur la longueur de ce guide d'ondes. Les rayonnements centraux des signaux optiques se déplaçant à travers le guide d'ondes peuvent être réfractés vers des rayons plus élevés tandis que les rayonnements extérieurs se propagent sans être altérés. Le dispositif optique peut diminuer la dispersion des signaux optiques qui se déplacent à travers une fibre optique.
Applications Claiming Priority (2)
Application Number | Priority Date | Filing Date | Title |
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US201862665229P | 2018-05-01 | 2018-05-01 | |
US62/665,229 | 2018-05-01 |
Publications (1)
Publication Number | Publication Date |
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WO2019213163A1 true WO2019213163A1 (fr) | 2019-11-07 |
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PCT/US2019/030047 WO2019213163A1 (fr) | 2018-05-01 | 2019-04-30 | Dispositif de conditionnement de mode optique mmf |
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US (1) | US10795078B2 (fr) |
WO (1) | WO2019213163A1 (fr) |
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US10935720B2 (en) * | 2019-04-29 | 2021-03-02 | Ii-Vi Delaware, Inc. | Laser beam product parameter adjustments |
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US20070206912A1 (en) * | 2005-11-03 | 2007-09-06 | Aculight Corporation | Apparatus and method for a waveguide with an index profile manifesting a central dip for better energy extraction |
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US20110110627A1 (en) * | 2009-11-07 | 2011-05-12 | Dr. Chang Ching TSAI | Beam collimator |
WO2016178595A1 (fr) * | 2015-05-07 | 2016-11-10 | Huawei Technologies Co., Ltd. | Coupleur optique à guide d'ondes à gradient d'indice |
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FR2699293B1 (fr) * | 1992-12-15 | 1995-03-03 | France Telecom | Système optique monolithique comportant des moyens de couplage perfectionnés entre une fibre optique et un phototransducteur. |
US5719973A (en) * | 1996-07-30 | 1998-02-17 | Lucent Technologies Inc. | Optical waveguides and components with integrated grin lens |
FR2815421B1 (fr) * | 2000-10-16 | 2003-09-19 | France Telecom | Collimateur optique pour fibres monomodes, fibre monomode a collimateur integre et procede de fabrication |
JP2002196181A (ja) * | 2000-12-25 | 2002-07-10 | Nippon Sheet Glass Co Ltd | レンズ機能付き光ファイバおよびその製造方法 |
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CA2919002A1 (fr) * | 2013-07-22 | 2015-01-29 | Adc Telecommunications, Inc. | Ensemble cable et connecteur de fibre optique a faisceau elargi et procedes de fabrication associes |
JP6396696B2 (ja) * | 2014-06-26 | 2018-09-26 | 株式会社トプコン | 光波距離計 |
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-
2019
- 2019-04-30 US US16/399,140 patent/US10795078B2/en active Active
- 2019-04-30 WO PCT/US2019/030047 patent/WO2019213163A1/fr active Application Filing
Patent Citations (5)
Publication number | Priority date | Publication date | Assignee | Title |
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US4723828A (en) * | 1984-11-09 | 1988-02-09 | Northern Telecom Limited | Bandwidth enhancement of multimode optical transmisson lines |
US20070206912A1 (en) * | 2005-11-03 | 2007-09-06 | Aculight Corporation | Apparatus and method for a waveguide with an index profile manifesting a central dip for better energy extraction |
US7340138B1 (en) * | 2007-01-25 | 2008-03-04 | Furukawa Electric North America, Inc. | Optical fiber devices and methods for interconnecting dissimilar fibers |
US20110110627A1 (en) * | 2009-11-07 | 2011-05-12 | Dr. Chang Ching TSAI | Beam collimator |
WO2016178595A1 (fr) * | 2015-05-07 | 2016-11-10 | Huawei Technologies Co., Ltd. | Coupleur optique à guide d'ondes à gradient d'indice |
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US20190339454A1 (en) | 2019-11-07 |
US10795078B2 (en) | 2020-10-06 |
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